U.S. patent application number 11/912830 was filed with the patent office on 2009-02-05 for confocal microscope.
Invention is credited to Hisashi Okugawa.
Application Number | 20090034062 11/912830 |
Document ID | / |
Family ID | 38023089 |
Filed Date | 2009-02-05 |
United States Patent
Application |
20090034062 |
Kind Code |
A1 |
Okugawa; Hisashi |
February 5, 2009 |
CONFOCAL MICROSCOPE
Abstract
A confocal microscope apparatus is capable of obtaining a high
confocal effect while detecting an image of a specimen line by
line. The confocal microscope apparatus may include an illuminating
optical system which illuminates a line-shaped area on a specimen
plane in a specimen by collected light, an image-forming optical
system which forms an image of light emitted from the specimen
plane, a two-dimensional light detector which is placed at a
conjugate plane of the specimen plane, a scanning unit which moves
the line-shaped area on the specimen plane, and a correcting unit
which corrects a pixel signal of a specific line on the
two-dimensional light detector having a confocal relation with the
line-shaped area based on a pixel signal of a peripheral line of
the specific line.
Inventors: |
Okugawa; Hisashi;
(Kanagawa-ken, JP) |
Correspondence
Address: |
MILES & STOCKBRIDGE PC
1751 PINNACLE DRIVE, SUITE 500
MCLEAN
VA
22102-3833
US
|
Family ID: |
38023089 |
Appl. No.: |
11/912830 |
Filed: |
October 16, 2006 |
PCT Filed: |
October 16, 2006 |
PCT NO: |
PCT/JP2006/320589 |
371 Date: |
October 26, 2007 |
Current U.S.
Class: |
359/368 |
Current CPC
Class: |
G02B 21/0048 20130101;
G02B 21/008 20130101 |
Class at
Publication: |
359/368 |
International
Class: |
G02B 21/00 20060101
G02B021/00 |
Foreign Application Data
Date |
Code |
Application Number |
Nov 11, 2005 |
JP |
2005-327343 |
Claims
1. A confocal microscope apparatus, comprising: an illuminating
optical system which illuminates a line-shaped area on a specimen
plane in a specimen by collected light; an image-forming optical
system which forms an image of light emitted from said specimen
plane; a two-dimensional light detector which is placed at a
conjugate plane of said specimen plane; a scanning unit which moves
said line-shaped area on said specimen plane; and a correcting unit
which corrects a pixel signal of a specific line on said
two-dimensional light detector having a confocal relation with said
line-shaped area based on a pixel signal of a peripheral line of
the specific line.
2. The confocal microscope apparatus according to claim 1, wherein
in said peripheral line, at least a line adjacent to said specific
line is included.
3. The confocal microscope apparatus according to claim 2, wherein
said correcting unit corrects a jth pixel signal S.sub.(0,j) of
said specific line L.sub.0 at least based on (j.+-.1)th pixel
signals S.sub.(1,j+1), S.sub.(1,j-1) of a line L.sub.1 shifted by
one line from the specific line L.sub.0.
4. The confocal microscope apparatus according to claim 3, wherein
said correcting unit corrects the jth pixel signal S.sub.(0,j) of
said specific line L.sub.0 based on (j.+-.k)th pixel signals
S.sub.(k,j+k), S.sub.(k,j-k) of a line L.sub.k shifted by k lines
from said specific line L.sub.0 by a following equation. S ( 0 , j
) = S ( 0 , j ) - ( S ( 1 , j + 1 ) + S ( 1 , j - 1 ) ) - ( S ( 2 ,
j + 2 ) + S ( 2 , j - 2 ) ) - ( S ( 3 , j + 3 ) + S ( 3 , j - 3 ) )
##EQU00005##
5. The confocal microscope apparatus according to claim 1, wherein
in said peripheral line, at least two lines adjacent to both sides
of said specific line are included.
6. The confocal microscope apparatus according to claim 5, wherein
said correcting unit corrects a jth pixel signal S.sub.(0,j) of
said specific line L.sub.0 at least based on (j.+-.1)th pixel
signals S.sub.(1,j+1), S.sub.(-1,j+1), S.sub.(1,j-1),
S.sub.(-1,j-1) of two lines L.sub.1, L.sub.1 shifted by plus or
minus one line from the specific line L.sub.0.
7. The confocal microscope apparatus according to claim 6, wherein
said correcting unit corrects the jth pixel signal S.sub.(0,j) of
said specific line L.sub.0 based on (j.+-.k)th pixel signals
S.sub.(k,j+k), S.sub.(-k,j+k), S.sub.(k,j-k), S.sub.(-k,j-k) of
lines L.sub.+k, L.sub.-k shifted by plus or minus k lines from said
specific line L.sub.0 by a following equation. S ( 0 , j ) = S ( 0
, j ) - [ ( S ( 1 , j + 1 ) + S ( - 1 , j + 1 ) ) / 2 + ( S ( 1 , j
- 1 ) + S ( - 1 , j - 1 ) ) / 2 ] - [ ( S ( 2 , j + 2 ) + S ( - 2 ,
j + 2 ) ) / 2 + ( S ( 2 , j - 2 ) + S ( - 2 , j - 2 ) ) / 2 ] - [ (
S ( 3 , j + 3 ) + S ( - 3 , j + 3 ) ) / 2 + ( S ( 3 , j - 3 ) + S (
- 3 , j - 3 ) ) / 2 ] - ##EQU00006##
Description
CROSS-REFERENCE TO RELATED APPLICATION
[0001] This application is a 371 of International Application
Number PCT/JP2006/320589, filed Oct. 16, 2006, which claims the
priority of Japanese Application Number 2005-327343 filed Nov. 11,
2005.
TECHNICAL FIELD
[0002] The present invention relates to a confocal microscope
apparatus which detects an image of a specimen line by line.
BACKGROUND ART
[0003] Generally, a linescanning confocal microscope apparatus
illuminates a sample by illuminating light collected in a line
shape and detects light generated in an illuminated area on the
sample by a light detector such as a one-dimensional CCD (Patent
Document 1 or the like). To acquire a two-dimensional image, it is
only required to repeat detection while scanning the sample in the
illuminated area. If the detection is performed line by line as
just described, the time until two-dimensional image information is
acquired can be made shorter than an ordinary confocal microscope
apparatus which performs detection point by point. Patent Document
1: Japanese Unexamined Patent Application Publication No.
2000-275027
DISCLOSURE
Problems to be Solved
[0004] However, in a linescanning confocal microscope apparatus,
crosstalk regarding a short side direction of an illuminated area
is suppressed, but crosstalk regarding a longitudinal direction
thereof is not suppressed, so that in observation of a sample
distributed in the longitudinal direction, a confocal effect
(sectioning resolution in a light axis direction and contrast in a
planar direction) cannot be obtained.
[0005] Hence, an object of the present invention is to provide a
confocal microscope apparatus capable of obtaining a high confocal
effect while detecting an image of a specimen line by line.
Means for Solving the Problems
[0006] A confocal microscope apparatus of the present invention
includes: an illuminating optical system which illuminates a
line-shaped area on a specimen plane in a specimen by collected
light; an image-forming optical system which forms an image of
light emitted from the specimen plane; a two-dimensional light
detector which is placed at a conjugate plane of the specimen
plane; a scanning unit which moves the line-shaped area on the
specimen plane; and a correcting unit which corrects a pixel signal
of a specific line on the two-dimensional light detector having a
confocal relation with the line-shaped area based on a pixel signal
of a peripheral line of the specific line.
[0007] Incidentally, it is desirable that in the peripheral line,
at least a line adjacent to the specific line be included.
[0008] Further, it is recommended that the correcting unit correct
a jth pixel signal S.sub.(0,j) of the specific line L.sub.0 at
least based on (j.+-.1)th pixel signals S.sub.(1,j+1),
S.sub.(1,j-1) of a line L.sub.1 shifted by one line from the
specific line L.sub.0.
[0009] Furthermore, the correcting unit may correct the jth pixel
signal S.sub.(0,j) of the specific line L.sub.0 based on (j.+-.k)th
pixel signals S.sub.(k,j+k), S.sub.(k,j-k) of a line L.sub.k
shifted by k lines from the specific line L.sub.0 by a following
equation.
S ( 0 , j ) = S ( 0 , j ) - ( S ( 1 , j + 1 ) + S ( 1 , j - 1 ) ) -
( S ( 2 , j + 2 ) + S ( 2 , j - 2 ) ) - ( S ( 3 , j + 3 ) + S ( 3 ,
j - 3 ) ) ##EQU00001##
[0010] Moreover, it is desirable that in the peripheral line, at
least two lines adjacent to both sides of the specific line be
included.
[0011] Further, the correcting unit may correct a jth pixel signal
S.sub.(0,j) of the specific line L.sub.0 at least based on
(j.+-.1)th pixel signals S.sub.(1,j+1), S.sub.(-1,j+1),
S.sub.(1,j-1), S.sub.(-1,j-1) of two lines L.sub.1, L.sub.-1
shifted by plus or minus one line from the specific line
L.sub.0.
[0012] Furthermore, the correcting unit may correct the jth pixel
signal S.sub.(0,j) of the specific line L.sub.0 based on (j.+-.k)th
pixel signals S.sub.(k,j+k), S.sub.(-k,j+k), S.sub.(-k,j-k),
S.sub.(-k,j-k) of lines L.sub.k, L.sub.-k shifted by plus or minus
k lines from the specific line L.sub.0 by a following equation.
S ( 0 , j ) = S ( 0 , j ) - [ ( S ( 1 , j + 1 ) + S ( - 1 , j + 1 )
) / 2 + ( S ( 1 , j - 1 ) + S ( - 1 , j - 1 ) ) / 2 ] - [ ( S ( 2 ,
j + 2 ) + S ( - 2 , j + 2 ) ) / 2 + ( S ( 2 , j - 2 ) + S ( - 2 , j
- 2 ) ) / 2 ] - [ ( S ( 3 , j + 3 ) + S ( - 3 , j + 3 ) ) / 2 + ( S
( 3 , j - 3 ) + S ( - 3 , j - 3 ) ) / 2 ] - ##EQU00002##
EFFECT
[0013] According to the present invention, a confocal microscope
apparatus capable of obtaining a high confocal effect while
detecting an image of a specimen line by line is realized.
BRIEF DESCRIPTION OF THE DRAWINGS
[0014] FIG. 1 is an overall configuration diagram of the present
microscope apparatus;
[0015] FIG. 2 is a diagram showing a state in which a sample 8 is
illuminated in a magnified form;
[0016] FIG. 3 schematically depicts a light path from the sample 8
to an imaging plane 10a;
[0017] FIG. 4 is a schematic diagram of the imaging plane 10a
viewed from the front;
[0018] FIG. 5 is a diagram explaining crosstalk occurring among
pixels in a specific line L.sub.0;
[0019] FIG. 6 is a diagram showing images which affect some pixel
P.sub.(0,0) on the specific line L.sub.0;
[0020] FIG. 7 is a diagram showing a general pixel P.sub.(0,j) on
the specific line L.sub.0 and pixels representing crosstalk
components of its pixel signal; and
[0021] FIG. 8 is an operational flowchart of a computer 11.
DETAILED DESCRIPTION OF THE EMBODIMENTS
First Embodiment
[0022] An embodiment of the present invention will be described
below with reference to the drawings. This embodiment is an
embodiment of a confocal microscope apparatus.
[0023] First, the overall configuration of this microscope
apparatus will be described.
[0024] FIG. 1 is an overall configuration diagram of this
microscope apparatus. As shown in FIG. 1, in this microscope
apparatus, a laser light source 1, a cylindrical lens 3, a beam
splitter 4, a lens 5, a scanner 6, an objective lens 7, a sample
(such as an organism sample) 8, a two-dimensional CCD 10, a
computer 11, a monitor 12, and so on are placed.
[0025] Laser light 2 emitted from the laser light source 1 is
collected in a line shape by the cylindrical lens 3. After passing
through the beam splitter 4, the laser light 2 is converted into
parallel light by the lens 5, reflected by a scanning mirror 6a in
the scanner 6, and collected in a line-shaped area (illuminated
area) E on the sample 8 via the objective lens 7.
[0026] Light generated in the illuminated area E returns to the
beam splitter 4 via the objective lens 7, the scanning mirror 6a,
and the lens 5. This light is reflected by the beam splitter 4 and
forms an image of the illuminated area E at a specific line L.sub.0
on an imaging plane 10a of the two-dimensional CCD 10. The
two-dimensional CCD 10 detects a brightness distribution of the
imaging plane 10a to generate brightness distribution data and
sends it to the computer 11.
[0027] Incidentally, the scanner 6 can change a placement angle of
the scanning mirror 6a and moves the illuminated area E on the
sample 8 in a short side direction (scanning direction) DS thereof.
When the illuminated area E moves on the sample 8 as just
described, an image of a different line on the sample 8 is
projected on the specific line L.sub.0 of the two-dimensional CCD
10.
[0028] Further, the laser light source 1, the scanner 6, the
two-dimensional CCD 10, and so on are controlled by the computer
11. For example, the computer 11 performs control processing of
controlling the two-dimensional CCD 10 to acquire the brightness
distribution data while controlling the scanner 6 to scan the
sample 8 in the illuminated area E (details of which will be
described later). Further, the computer 11 performs arithmetical
processing of processing the acquired brightness distribution data
to generate a two-dimensional image of the sample 8 (details of
which will be described later). Furthermore, the computer 11 also
performs conversion processing to display this image on the monitor
12, and the like.
[0029] FIG. 2 is a diagram showing a state in which the sample 8 is
illuminated in a magnified form. Illuminating light is collected on
a specimen plane 8a in the sample 8 and has spreads in an upper
layer and a lower layer of the specimen plane 8a. Hence,
hereinafter, the illuminated area E on the specimen plane 8a is
particularly called an "illuminated line E".
[0030] FIG. 3 schematically depicts a light path from the sample 8
to the imaging plane 10a. In FIGS. 3(A), (B), states in which the
light path is seen from angles different by 90.degree. are
shown.
[0031] As shown in FIGS. 3(A), (B), the imaging plane 10a is
located at a conjugate plane of the specimen plane 8a, and the
specific line L.sub.0 of the imaging plane 10a has a confocal
relation with the illuminated line E. Light generated at one point
on the illuminated line E is collected on the specific line L.sub.0
and forms an image of the point on one pixel of the specific line
L.sub.0. Namely, images of respective points on the illuminated
line E are formed on respective pixels of the specific line
L.sub.0.
[0032] However, in actuality, light (flare) is generated also in
lines E' in an upper layer and a lower layer of the illuminated
line E. Flare generated at one point on the line E' is collected
before or behind the specific line L.sub.0, so that an blurred
image of the point is formed on plural pixels of the specific line
L.sub.0. Namely, on the respective pixels of the specific line
L.sub.0, blurred images of respective points on the line E' are
overlappingly formed.
[0033] As a result, in each pixel of the specific line L.sub.0,
crosstalk regarding a scanning direction DS does not occur, but
crosstalk regarding a line direction DL occurs.
[0034] Next, the crosstalk regarding the line direction DL will be
described in detail.
[0035] FIG. 4 is a schematic diagram of the imaging plane 10a
viewed from the front. As shown in FIG. 4, the specific line
L.sub.0 is located near the center of the imaging plane 10a. In the
lower part of FIG. 4, the specific line L.sub.0 and part of
peripheral lines of the specific line are shown in a magnified
form. Hereinafter, as shown in FIG. 4, a line shifted by i lines
from the specific line L.sub.0 is called a "line L.sub.i".
[0036] Shown on the left side of FIG. 5 is a schematic diagram of a
section of part of the sample 8, and shown on the right side
thereof is a schematic diagram of the imaging plane 10a. In FIG. 5,
a light axis direction is represented by the symbol Z, and line
directions of the illuminated line E and the specific line L.sub.0
are represented by the symbol DL.
[0037] When some point A.sub.00 on the illuminated line E forms an
image A.sub.00' on a minute circular area on the specific line
L.sub.0 of the imaging plane 10a as shown in FIG. 5(A), points
A.sub.01 in an upper layer and a lower layer of the point A.sub.00
form a blurred image A.sub.01' with the same point as the image
A.sub.00' as its center and cause crosstalk to pixels within its
formation range. Further, points A.sub.02 in an upper layer and a
lower layer of the points A.sub.01 form a more blurred image
A.sub.02' with the same point as the image A.sub.00' as its center
and cause crosstalk to pixels within its formation range.
[0038] Namely, points A.sub.01, A.sub.02, . . . in an upper layer
and a lower layer of the point A.sub.00 form blurred images
A.sub.01', A.sub.02', . . . with the same point as the image
A.sub.00' as their center and cause crosstalk to pixels in their
formation ranges. Incidentally, the more blurred the image, the
smaller the crosstalk quantity given to one pixel becomes.
[0039] The same goes for a different point on the illuminated line
E and points in the upper layer and the lower layer (see FIGS.
5(B), (C)). In FIGS. 5(B), (C), as in FIG. 5(A), the same
subscripts are given to points A in the sample 8 and the images A'
on the imaging plane 10a which correspond to each other.
[0040] Next, crosstalk components occurring in a pixel signal of
the specific line L.sub.0 will be described.
[0041] In FIG. 6, attention is paid to some pixel P.sub.(0,0) on
the specific line L.sub.0, and only images which affect the pixel
P.sub.(0,0) are shown. Incidentally, P.sub.(i,j) is a jth pixel of
a line L.sub.i.
[0042] As shown in FIG. 6, the image A.sub.00' formed on the pixel
P.sub.(0,0) and images A.sub.11', A.sub.-11', A.sub.22',
A.sub.-22', . . . each of which has its center at a position (mark
X) shifted from the pixel P.sub.(0,0) in the line direction DL and
blurred by its shift quantity affect the pixel P.sub.(0,0).
[0043] Among them, the image A.sub.00' is an image to be detected
by the pixel P.sub.(0,0) and an image generating a signal component
with respect to the pixel P.sub.(0,0). The other images A.sub.11',
A.sub.22', A.sub.-11', A.sub.-22', . . . generate crosstalk
components with respect to the pixel P.sub.(0,0).
[0044] Here, the crosstalk quantity given to the pixel P.sub.(0,0)
by the image A.sub.11' is regarded as appearing in a pixel signal
of a pixel P.sub.(1,1) or a pixel P.sub.(-1,1) arranged in an
oblique direction with respect to the pixel P.sub.(0,0).
[0045] This is because, firstly, the crosstalk quantities of the
pixels P.sub.(1,1), P.sub.(-1,1) received from the image A.sub.11'
are each the same as that of the pixel P.sub.(0,0). Secondly, the
pixels P.sub.(1,1), P.sub.(-1,1) exist on lines off the specific
line L.sub.0, and hence have no signal component.
[0046] By thinking in the same way, the crosstalk quantity given to
the pixel P.sub.(0,0) by the image A.sub.-11' is regarded as
appearing in a pixel signal of a pixel P.sub.(1,-1) or a pixel
P.sub.(-1,-1).
[0047] Further, the crosstalk quantity applied to the pixel
P.sub.(0,0) by the image A.sub.22' is regarded as appearing in a
pixel signal from a pixel P.sub.(2,2) or a pixel P.sub.(-2,2).
[0048] Furthermore, the crosstalk quantity given to the pixel
P.sub.(0,0) by the image A.sub.-22' is regarded as appearing in a
pixel signal of a pixel P.sub.(2,-2) or a pixel P.sub.(-2,-2).
[0049] Accordingly, pixel signals S.sub.(1,1), S.sub.(-1,1),
S.sub.(1,-1) S.sub.(-1,-1), S.sub.(2,2), S.sub.(-2,2),
S.sub.(2,-2), S.sub.(-2, -2), . . . of the pixels P.sub.(1,1),
P.sub.(-1,1), P.sub.(1,-1) P.sub.(-1,-1), P.sub.(2,2),
P.sub.(-2,2), P.sub.(2,-2), P.sub.(-2,-2), . . . represent
crosstalk components contained in a pixel signal S.sub.(0,0) of the
pixel P.sub.(0,0).
[0050] Incidentally, the P.sub.(1,1) and the P.sub.(-1,1), the
pixel P.sub.(1,-1) and the pixel P.sub.(-1,-1), and the like have a
symmetrical relation with respect to the specific line L.sub.0, so
that in principle, they should output the same pixel signal. If a
difference occurs between the two pixel signals, it is due to the
influence of noise. Accordingly, a mean value (mean pixel signal)
of the two pixel signals more accurately represents the crosstalk
component.
[0051] Further, the larger the blur quantity of one image A', the
smaller the crosstalk quantity given to one pixel by this image A'
becomes, so that out of the pixels P.sub.(1,1), P.sub.(-1,1),
P.sub.(1,-1) P.sub.(-1,-1), P.sub.(2,2), P.sub.(-2,2),
P.sub.(2,-2), P.sub.(-2,-2), . . . , a pixel on a line closer to
the specific line L.sub.0 represents a more dominant crosstalk
component with respect to the pixel P.sub.(0,0).
[0052] Moreover, the above description applies to each of pixels on
the specific line L.sub.0. In FIG. 7, a general pixel P.sub.(0,j)
on the specific line L.sub.0 and pixels representing crosstalk
components contained in a pixel signal S.sub.(0,j) of the pixel
P.sub.(0,j) are shown using a general pixel number "j". Out of
these pixels, an average pixel signal of two pixels symmetrical
with respect to the specific line L.sub.0 more accurately
represents the crosstalk component. Further, a pixel on a line
closer to the specific line L.sub.0 represents a more dominant
crosstalk component with respect to the pixel P.sub.(0,j).
[0053] Next, based on the above, the operation of the computer 11
of this microscope apparatus will be described in detail.
[0054] FIG. 8 is an operational flowchart of the computer 11.
Respective steps will be sequentially described.
[0055] (Step S1)
[0056] The computer 11 synchronously controls the scanner 6 and the
two-dimensional CCD shown in FIG. 1, and while scanning the sample
8 in the illuminated area E, acquires brightness distribution data
when the illuminated area E is on respective lines on the sample 8,
respectively (step S1). N brightness distribution data acquired
here are taken as I.sub.1, I.sub.2, I.sub.3, . . . , I.sub.N in
order of acquisition.
[0057] A specific pixel signal string S.sub.0 contained in each of
the brightness distribution data I.sub.1, I.sub.2, I.sub.3, . . . ,
I.sub.N is a pixel signal string from the above specific line
L.sub.0. Information on lines different from one another on the
sample 8 is reflected in the pixel signal string S.sub.0 of the
brightness distribution data I.sub.1, the pixel signal string
S.sub.0 of the brightness distribution data I.sub.3, the pixel
signal string S.sub.0 of the brightness distribution data I.sub.3,
. . . , the pixel signal string S.sub.0 of the brightness
distribution data I.sub.N.
[0058] (Step S2)
[0059] The computer 11 refers to the pixel signal string S.sub.0 of
the brightness distribution data I.sub.1 and its peripheral pixel
signal strings S.sub.1, S.sub.-1, S.sub.2, S.sub.-2, . . . and
corrects the former based on the latter. Incidentally, the pixel
signal string S.sub.i is a pixel signal string of a line L.sub.i,
and a pixel signal S.sub.(l,j) in the pixel signal string S.sub.i
is a pixel signal of a pixel P.sub.(l,j).
[0060] In this correction, each pixel signal S.sub.(0,j) in the
pixel signal string S.sub.0 is corrected by the following equation
(1).
S ( 0 , j ) = S ( 0 , j ) - [ ( S ( 1 , j + 1 ) + S ( - 1 , j + 1 )
) / 2 + ( S ( 1 , j - 1 ) + S ( - 1 , j - 1 ) ) / 2 ] - [ ( S ( 2 ,
j + 2 ) + S ( - 2 , j + 2 ) ) / 2 + ( S ( 2 , j - 2 ) + S ( - 2 , j
- 2 ) ) / 2 ] - [ ( S ( 3 , j + 3 ) + S ( - 3 , j + 3 ) ) / 2 + ( S
( 3 , j - 3 ) + S ( - 3 , j - 3 ) ) / 2 ] - ( 1 ) ##EQU00003##
[0061] In the right side of this equation (1), each term in square
brackets is a correcting term.
[0062] The first correcting term in equation (1) means a correction
by four pixels P.sub.(1,j+1), P.sub.(-1,j+1), P.sub.(1,j-1),
P.sub.(-1,j-1) on lines L.sub.1, L.sub.-1 shifted by one line from
the specific line L.sub.0 (see FIG. 7).
[0063] The second correcting term in equation (1) means a
correction by four pixels P.sub.(2,j+2), P.sub.(-2,j+2),
P.sub.(2,j-2), P.sub.(-2,j-2) on lines L.sub.2, L.sub.-2 shifted by
two lines from the specific line L.sub.0 (see FIG. 7).
[0064] Similarly, the kth correcting term in equation (1) means a
correction by four pixels P.sub.(k,j+k), P.sub.(-k,j+k),
P.sub.(k,j-k), P.sub.(-k,j-k) on lines L.sub.k, L.sub.-k shifted by
k lines from the specific line L.sub.0.
[0065] Hence, according to the first correcting term, the most
dominant crosstalk components in the pixel signal S.sub.(0,j) are
removed, according to the second correcting term, the second most
dominant crosstalk components in the pixel signal S.sub.(0,j) are
removed, and according to the kth correcting term, the kth most
dominant crosstalk components in the pixel signal S.sub.(0,j) are
removed.
[0066] Further, (S.sub.(k,j+k)+S.sub.(-k,j+k))/2 in the kth
correcting term represents a mean pixel signal of two pixels
P.sub.(k,j+k), P.sub.(-k,j+k)) symmetrical with respect to the
specific line L.sub.0. Therefore, according to respective
correcting terms in equation (1), various crosstalk components can
be removed with high accuracy, respectively.
[0067] Incidentally, the number of correcting terms in equation (1)
may be set to a small number such as two or one. This is because
the larger kth correcting term (that is, the line more distant from
the specific line L.sub.0) has a weaker correcting effect. If the
number of correcting terms can be kept low, the number of pixel
signal strings to be referred to by the computer 11 in step S2 and
arithmetical loading of the computer 11 can be reduced. On the
other hand, it is possible in principle to increase the correcting
accuracy as the number of correcting terms is increased, but in
actuality, the larger kth correcting term (that is, the line more
distant from the specific line L.sub.0) has worse S/N, and hence if
the number of correcting terms is too many, the correcting accuracy
may inversely deteriorate. Therefore, it is desirable to select an
optimum value as the number of correcting terms by prior
experiment, simulation, and so on.
[0068] Similarly, the computer 11 corrects a pixel signal string
S.sub.0 of the brightness distribution data I.sub.2 based on its
peripheral pixel signal strings S.sub.1, S.sub.-1, S.sub.2,
S.sub.-2, . . . . Similarly, the computer 11 also corrects pixel
signal strings S.sub.0 of the brightness distribution data I.sub.3,
I.sub.4, I.sub.5, I.sub.6, . . . , I.sub.N.
[0069] Incidentally, in this step described above, the corrected
pixel signal string S.sub.0 obtained from the bright data I.sub.1
is replaced with S.sub.10, the corrected pixel signal string
S.sub.0 obtained from the bright data I.sub.2 with S.sub.20, . . .
, and the corrected pixel signal string S.sub.0 obtained from the
bright data I.sub.N with S.sub.N0.
[0070] (Step S3)
[0071] The computer 11 arranges and combines the corrected pixel
signal strings S.sub.10, S.sub.20, S.sub.30, . . . S.sub.N0 in this
order to create one image data I. This image data I represents a
two-dimensional image of the sample 8.
[0072] As described above, this microscope apparatus is a
linescanning confocal microscope apparatus, and hence the crosstalk
regarding the scanning direction DS does not occur, but the
crosstalk regarding the line direction DL occurs. However, in this
microscope apparatus, a two-dimensional brightness distribution
containing not only the specific line L.sub.0 corresponding to the
illuminated line E and but also peripheral lines of the specific
line is detected, and the former pixel signal is corrected based on
the latter pixel signals. The crosstalk regarding the line
direction DL is suppressed by this correction. Accordingly, this
microscope apparatus can obtain a high confocal effect although it
is the linescanning one.
[0073] Besides, the computer 11 of this microscope apparatus uses
the mean pixel signal of two pixels symmetrical with respect to the
specific line L.sub.0 in the correction (see equation (1)), so that
its correcting accuracy can be increased.
[0074] (Others)
[0075] Further, in the correction in step S2, equation (2) may be
used instead of equation (1).
S ( 0 , j ) = S ( 0 , j ) - ( S ( 1 , j + 1 ) + S ( 1 , j - 1 ) ) -
( S ( 2 , j + 2 ) + S ( 2 , j - 2 ) ) - ( S ( 3 , j + 3 ) + S ( 3 ,
j - 3 ) ) - ( 2 ) ##EQU00004##
[0076] In the right side of this equation (2), each term in
parentheses is a correcting term.
[0077] The first correcting term in equation (2) means a correction
by two pixels P.sub.(1,j+1), P.sub.(1,j-1) on L.sub.1 shifted by
one line from the specific line L.sub.0 (see FIG. 7).
[0078] The second correcting term in equation (2) means a
correction by two pixels P.sub.(2,j+2), P.sub.(2,j-2) on the line
L.sub.2 shifted by two lines from the specific line L.sub.0 (see
FIG. 7).
[0079] Similarly, the kth correcting term in equation (2) means a
correction by two pixels P.sub.(k,j+k), P.sub.(k,j-k) on the line
L.sub.k shifted by k lines from the specific line L.sub.0.
[0080] Namely, in equation (2), the number of lines used for a
correction corresponds to half of that in equation (1). In this
equation (2), arithmetic to calculate the mean pixel signal is not
included, so that the speed of correcting arithmetic can be
increased.
[0081] Incidentally, also when equation (2) is used, the number of
correcting terms may be set to a small number such as two or one.
This is because the larger kth correcting term (that is, the line
more distant from the specific line L.sub.0) has a weaker
correcting effect. If the number of correcting terms can be kept
low, the number of pixel signal strings to be referred to by the
computer 11 in step S2 and arithmetical loading of the computer 11
can be reduced. On the other hand, it is possible in principle to
increase the accuracy as the number of correcting terms is
increased, but in actuality, the larger kth correcting term (that
is, the line more distant from the specific line L.sub.0) has worse
S/N, and hence if the number of correcting terms is too many, the
correcting accuracy may inversely deteriorate. Therefore, it is
desirable to select an optimum value as the number of correcting
terms by prior experiment, simulation, and so on.
[0082] Further, in this embodiment, no mention is made of the size
of the imaging plane 10a, but when the number of lines used for the
correction is small, the size of the imaging plane 10a of the
two-dimensional CCD may be correspondingly reduced.
[0083] For example, when equation (1) is used as a correcting
equation and the number of its correcting terms is two, only four
lines are used for the correction, and therefore, the imaging plane
10a has only to have five lines of the specific line L.sub.0 and
lines L.sub.1, L.sub.1, L.sub.2, L.sub.-2.
[0084] Furthermore, when equation (2) is used as the correcting
equation and the number of its correcting terms is two, only two
lines are used for the correction, and therefore, the imaging plane
10a has only to have three lines of the specific line L.sub.0 and
lines L.sub.1, L.sub.2.
[0085] Moreover, in this microscope apparatus, the two-dimensional
CCD is used as a two-dimensional light detector, but a different
type of two-dimensional light detector may be used as long as it
can detect a brightness distribution formed simultaneously in the
specific line and peripheral lines of the specific line.
[0086] Additionally, this microscope apparatus applies the present
invention to the linescanning confocal microscope, but even in the
case of a spotscanning confocal microscope, the application of the
present invention becomes effective as the case may be. It is a
case where spotscanning is speeded up and an image of a sample is
detected line by line by a charge storage light detector such as a
CCD. The charge storage light detector detects the time integral of
light intensity incident within a finite time period, and hence,
even lights incident on different positions on the CCD at different
timings cause crosstalk to each other's signals when their incident
timings fall within the charge storage period of the CCD. However,
the application of the present invention can suppress this
crosstalk.
[0087] Further, using this microscope apparatus, fluorescence may
be observed. For reference's sake, in the fluorescence observation,
it is only required to place a sample labeled by a fluorescent
material as the sample 8, place a dichroic mirror as the beam
splitter 4, and place a filter as necessary in an appropriate
position around the dichroic mirror.
[0088] Furthermore, part or all of processing by the computer 11 of
this microscope apparatus may be executed by a circuit instead of
the computer 11. The use of the circuit makes it possible to
shorten the time until a confocal image is displayed.
[0089] The many features and advantages of the invention are
apparent from the foregoing description. It is to be understood
that the invention is not limited to the described embodiments,
which are intended to be illustrative and not limiting. As will
readily occur to those skilled in the art, numerous changes and
modifications are possible in keeping with the principles and
spirit of the invention, the scope of which is defined in the
appended claims.
* * * * *